Wavelength-division-multiplexing (WDM) technology has been developing in broadband optical networks. The wavelength range used in fiber transmission systems has been increasing by employing various kinds of fiber amplifiers. In order to make it possible to handle signals of multiple wavelengths efficiently in network nodes, wavelength-selective processing in switching, routing and buffering systems will be required. In such processing systems, integrated-optic switches become one of fundamental key devices. In particular, high-speed wavelength-selective switches are required for WDM packet processing.
Wavelength-selective switches are classified from viewpoint of control method into electrically controlled devices and optically controlled ones. The former includes collinear acoustooptic (AO) devices (Goto & Miyazaki, 1990). Although multiple signals at different wavelengths can be independently switched with a single AO switch, it provides a response time only at an order of micro seconds. Optical circuits consisting of arrayed waveguide gratings (AWGs) and wavelength-insensitive switches are also regarded as a device in this class (Goh et al., 2008). The switching response depends on the control mechanizm of the wavelength-insensitive switches. The response time in thermo-optic switches is an order of milli seconds (Suzuki et al., 1998). On the other hand, optically controlled switches include devices using phase shift induced by optical nonlinear Kerr effect (Doran & Wood, 1988) and phase shift in semiconductor optical amplifiers (SOAs) (Nakamura et al., 2000) and in quantum dots (Kitagawa et al., 2009). These switches using phase shifting, in general, cannot provide wavelength-selectivity. Therefore, to realize wavelength-selective switching of the latter class, combination with multiplexers and demultiplexers such as AWGs is required.
As a switch of the latter class, the authors have proposed a new type of wavelength-selective switch where optical amplitudes in waveguide arms of interferometers are controlled by Raman amplifiers (Kishikawa & Goto, 2005; Kishikawa & Goto, 2006; Kishikawa & Goto, 2007a; Kishikawa & Goto, 2007b). In this article, the operation principle of wavelength-selective switching with the proposed devices is described. Computer simulation by finite-difference beam-propagation-method (FD-BPM) is performed to verify the switching operation.
2. Wavelength-selective switching by light control
Optical switching circuits discussed in this article consist of directional couplers, waveguide-type Raman amplifiers and attenuators as shown in Fig. 1. Designing of the switching circuits indicated by the dotted rectangular is theoretically discussed in the next section. In the switching circuits, the signal light intensity is controlled with waveguide-type Raman amplifiers. We consider that WDM optical signals at wavelengths λ 1, λ 2 and λ 3 are incident into the upper waveguide of the circuit, and the two signals at λ 1 and λ 3 are to be switched to OUT B, whereas the signal at λ 2 is to be forwarded to OUT A. To induce this routing operation, optical pumping signals at λ 1' and λ 3' are injected to Raman amplifiers, where λ
The wavelength-selective amplification can be performed in wide wavelength range by employing stimulated Raman scattering as shown in Fig. 2. The Raman gain bandwidth Δ
We denote the wavelength range available for this device as Δλtotal. Then, the WDM number handled with this switch is expressed as
2. Theoretical analysis of switching
2.1. Key elements
This section describes theoretical analysis with ideal device models. Key elements consisting the proposed switch are a 3-dB directional coupler and parallel independent waveguides containing amplifiers or attenuators as shown in Fig. 3. In the 3-dB directional coupler shown in (a), the electric field amplitude
Optical waves propagated along the independent parallel waveguides with amplification coefficient α 1 and α 2 are expressed as
2.2. Switch A
We have proposed two switch architectures. Figure 4 shows the device structure of one of the switch architectures, named as switch A. The switch consists of two cascaded interferometers. In the first interferometer, each arm has a Raman amplifier with amplification coefficient αA and αB for the lower and upper arms, respectively. An attenuator with attenuation coefficient β is placed in the upper arm of the second interferometer. The Raman amplifiers are pumped by backward traveling light coupled with polarization-selective or wavelength-selective couplers.
Optical WDM signals at wavelength λ
Using eqs.(2) and (3), the output fields through the switch are related to the input fields as
Since the incident optical signal is coupled into the lower port
By substituting eq. (5) into eq. (4), the outputs are obtained as
It is expected from eq. (6) that
It is found from eq.(7) that the switch operates as a 1x2 spatial switch whose output port is selected by proper amplification and attenuation effects. It is noted that the value
2.3. Switch B
An alternative architecture of the switch consists of cascaded three interferometers as shown in Fig. 5. Three Raman amplifiers are placed in the lower arms of the three interferometers. The feature of this architecture is that optical incident signals are routed to output port
Since the incident optical signal is coupled into the lower port
By substituting eq. (9) into eq. (8), the outputs are obtained as
For no amplification at each Raman amplifier, that is α=1, output electric fields are calculated to be
The difference of the output intensity by a factor of (6.222)2 can be compensated by employing an attenuator at output port
3. Numerical simulation of switching
3.1. Switch A
The switching characteristics can be analyzed using the equations described in the previous section. Wavelength dependence is also found by using eq. (1) instead of eq.(2) in the similar manner as described above. In this section, on the contrary, we verify the switching operation by numerical simulation to clarify the wave propagation along the waveguides of the switch. We use FD-BPM simulation with seventh-order Pade approximation (Hadley, 1992).
We consider a two-dimensional slab waveguide model as shown in Fig. 6. The step length and the step width in the lateral direction are Δ
The switching operation at λ=1550 nm is confirmed as shown in Fig.7, where squared electric fields |
The wavelength dependence of the output intensity with the switch is plotted in Fig. 8. At the designed wavelength λ=1550 nm, the switching extinction ratio is larger than 35 dB. The wavelength range to achieve an extinction ratio larger than 20 dB is approximately 40 nm, though the 10-dB extinction ration is obtained over 100 nm. This wavelength dependence is caused by the wavelength dependence of the directional couplers.
3.2. Switch B
The switching operation with switch B is also verified by FD-BPM simulation. The model used in the simulation is shown in Fig. 9. The total length of the switch is
The switching operation at λ=1550 nm is confirmed as shown in Fig. 10. Although the output intensities from output port
The wavelength dependence is shown in Fig. 11. At the designed wavelength λ=1550nm, the switching extinction ratio is larger than 25 dB. The wavelength range to achieve the extinction ratio larger than 20 dB is approximately 30 nm, though the 10-dB extinction ration is obtained over 80 nm.
4. Improvement of wavelength dependency
Waveguide-type Raman amplifiers do not depend on wavelength bands to be used because stimulated Raman scattering which is the base effect of Raman amplification can occur at any wavelength bands. Meanwhile, 3dB couplers have wavelength dependency in general, that is, the function of dividing an incident optical wave into two waves at the rate of 50:50 is available at some particular wavelength bands. The main cause of the wavelength dependency is the wavelength dependence of the coupling coefficient κ in eq.(1). For improving the characteristics of wavelength dependency of the switch and utilizing it at any wavelength bands, wavelength-independent (or wavelength-flattened) optical couplers should be employed. Fiber-type wavelength-independent couplers, that can be used for 50:50 of the dividing rate at wavelength bands such as 1550 nm± 40 nm and 1310 nm ± 40 nm, have already been on the market. However, waveguide-type wavelength-independent couplers have advantage from the viewpoint of integrating the switch elements.
An alternative for improving wavelength dependence is to replace the directional couplers by asymmetric X-junction couplers (Izutsu et al., 1982; Burns & Milton, 1980; Hiura et al., 2007). The asymmetric X-junction coupler has basically no dependence on wavelength and helps to improve the wavelength dependency of the proposed switch (Kishikawa et al., 2009a; Kishikawa et al., 2009b).
5. Another issue in implementation
Phase shift of the signal pulse experienced in the waveguide-type Raman amplifiers should be discussed because it can impact the operation of the switch. The phase shift is induced from refractive index change caused by self-phase modulation (SPM), cross-phase modulation (XPM), free carriers generated from two-photon absorption (TPA) (Roy et al., 2009), and temperature change. Although the structure of the switch becomes more complex, the effect of SPM and TPA-induced free carriers can be cancelled by installing the same nonlinear waveguides as those of the waveguide-type Raman amplifiers into counter arms of the Mach-Zehnder interferometers of the switch. The influence of XPM and temperature change involved with high power pump injection can also be suppressed by injecting pump waves, having the same power and different wavelengths that do not amplify the signal pulse, into the counterpart nonlinear waveguides.
We proposed a novel all-optical wavelength-selective switching having potential of a few tens of picosecond or faster operating speed. We discussed the theory and the simulation results of the switching operation and the characteristics. Moreover, the dynamic range over 25dB was also obtained from the simulation results of the switch. This characteristics can be wavelength-selective switching operation. More detailed analysis and simulation taking the nonlinearity of Raman amplifiers into account are required to confirm the operation with actual devices.
Although the principle and the fundamental verification were performed with the switches consisting of directional couplers, the idea can be similarly applied to switches consisting of other components such as asymmetric X-junction couplers to increase the wavelength range.